{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:7JWWDDF4VMIUDAPEM4MN3ZYBZW","short_pith_number":"pith:7JWWDDF4","schema_version":"1.0","canonical_sha256":"fa6d618cbcab114181e46718dde701cd8c9240420c4847eeadc4a938314bbeed","source":{"kind":"arxiv","id":"1702.00981","version":2},"attestation_state":"computed","paper":{"title":"Effective radius of ground- and excited-state positronium in collisions with hard walls","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. R. Swann, G. F. Gribakin, Q. Prigent, R. Brown","submitted_at":"2017-02-03T12:00:24Z","abstract_excerpt":"We determine effective collisional radii of positronium (Ps) by considering Ps states in hard-wall spherical cavities. $B$-spline basis sets of electron and positron states inside the cavity are used to construct the states of Ps. Accurate Ps energy eigenvalues are obtained by extrapolation with respect to the numbers of partial waves and radial states included in the bases. Comparison of the extrapolated energies with those of a pointlike particle provides values of the effective radius $\\rho_{nl}$ of Ps($nl$) in collisions with a hard wall. We show that for $1s$, $2s$, and $2p$ states of Ps,"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1702.00981","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-02-03T12:00:24Z","cross_cats_sorted":[],"title_canon_sha256":"5b946d4610d1555199d9ac448ed564a0903691cb5c4557a6a95234fa94b4273d","abstract_canon_sha256":"3ed1f24dc1fdefe048415bd8de2fc3762663302dd7fe4baf1ea80f3bf055b9df"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:48:09.252979Z","signature_b64":"qxEg2SJKcSDSzXITV/mt4Os1uqDPuGkuVt/23AIcKNq8MTawITICXPHRv4sEa5UG9+kwP+GAq1plCp+pZeOWDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fa6d618cbcab114181e46718dde701cd8c9240420c4847eeadc4a938314bbeed","last_reissued_at":"2026-05-18T00:48:09.252427Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:48:09.252427Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective radius of ground- and excited-state positronium in collisions with hard walls","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. R. Swann, G. F. Gribakin, Q. Prigent, R. Brown","submitted_at":"2017-02-03T12:00:24Z","abstract_excerpt":"We determine effective collisional radii of positronium (Ps) by considering Ps states in hard-wall spherical cavities. $B$-spline basis sets of electron and positron states inside the cavity are used to construct the states of Ps. Accurate Ps energy eigenvalues are obtained by extrapolation with respect to the numbers of partial waves and radial states included in the bases. Comparison of the extrapolated energies with those of a pointlike particle provides values of the effective radius $\\rho_{nl}$ of Ps($nl$) in collisions with a hard wall. We show that for $1s$, $2s$, and $2p$ states of Ps,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.00981","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1702.00981","created_at":"2026-05-18T00:48:09.252498+00:00"},{"alias_kind":"arxiv_version","alias_value":"1702.00981v2","created_at":"2026-05-18T00:48:09.252498+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.00981","created_at":"2026-05-18T00:48:09.252498+00:00"},{"alias_kind":"pith_short_12","alias_value":"7JWWDDF4VMIU","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_16","alias_value":"7JWWDDF4VMIUDAPE","created_at":"2026-05-18T12:31:05.417338+00:00"},{"alias_kind":"pith_short_8","alias_value":"7JWWDDF4","created_at":"2026-05-18T12:31:05.417338+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW","json":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW.json","graph_json":"https://pith.science/api/pith-number/7JWWDDF4VMIUDAPEM4MN3ZYBZW/graph.json","events_json":"https://pith.science/api/pith-number/7JWWDDF4VMIUDAPEM4MN3ZYBZW/events.json","paper":"https://pith.science/paper/7JWWDDF4"},"agent_actions":{"view_html":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW","download_json":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW.json","view_paper":"https://pith.science/paper/7JWWDDF4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1702.00981&json=true","fetch_graph":"https://pith.science/api/pith-number/7JWWDDF4VMIUDAPEM4MN3ZYBZW/graph.json","fetch_events":"https://pith.science/api/pith-number/7JWWDDF4VMIUDAPEM4MN3ZYBZW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW/action/storage_attestation","attest_author":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW/action/author_attestation","sign_citation":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW/action/citation_signature","submit_replication":"https://pith.science/pith/7JWWDDF4VMIUDAPEM4MN3ZYBZW/action/replication_record"}},"created_at":"2026-05-18T00:48:09.252498+00:00","updated_at":"2026-05-18T00:48:09.252498+00:00"}